US8755250B1ActiveUtility

Line array doppler processing

Individually held — no corporate assignee on recordPriority: Jun 7, 2011Filed: Jun 7, 2011Granted: Jun 17, 2014
Est. expiryJun 7, 2031(~4.9 yrs left)· nominal 20-yr term from priority
G01S 15/582G01S 11/10
60
PatentIndex Score
2
Cited by
6
References
4
Claims

Abstract

A method is taught to extract more information about the motion of an acoustic wave emitter moving relative to a line array of hydrophones that are part of a sonar system by determining the variation in Doppler shift across the entire line array of hydrophones together with the a range measurement of the emitter to calculate the emitter's velocity.

Claims

exact text as granted — not AI-modified
What is claimed is: 
     
       1. A method of determining the velocity of an underwater object moving parallel to an underwater line array of a plurality of N equally spaced acoustic sensors that are part of an active sonar system comprising:
 making contact with the underwater object with a narrow band continuous wave pulse from the active sonar system at a frequency f 0 ; 
 determining the range R of the object from the line array with a shorter pulse from the active sonar system centered at a frequency f 0 , wherein the time duration of the pulse is shorter than the time duration of the first narrow band continuous wave pulse; 
 receiving a frequency f N  at every acoustic sensor of the line array of N acoustic sensors; 
 calculating the frequency shift (T N −f 0 ) for each of the N individual acoustic sensors of the line array of N acoustic sensors; 
 plotting a line of frequency shift versus acoustic sensor for the measured Doppler shifts of a plurality of interior acoustic sensors to allow for confirmation of any difference in frequency using a linear least squares fit of the frequency shifts and to determine whether there is a measurable variation in the Doppler shift of the entire line array; 
 calculating the variation in Doppler shift of the entire line array of N acoustic sensors, based on the frequency shift of the first acoustic sensor and the Nth acoustic sensor of the line array of N acoustic sensors, expressed as 
 
       
         
           
             
               
                 
                   
                     Δ 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       f 
                       N 
                     
                   
                   - 
                   
                     Δ 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       f 
                       1 
                     
                   
                 
                 
                   f 
                   0 
                 
               
               ; 
             
           
         
       
       and
 determining the velocity of the underwater object according to the equation 
 
       
         
           
             
               
                 
                   
                     
                       Δ 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         f 
                         2 
                       
                     
                     - 
                     
                       Δ 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         f 
                         1 
                       
                     
                   
                   
                     f 
                     0 
                   
                 
                 ≅ 
                 
                   
                     v 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     Δ 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     θ 
                   
                   c 
                 
               
               , 
             
           
         
       
       wherein c is the speed of sound in water and wherein Δθ is equal to the length of the line array of N acoustic sensors divided by the range R of the underwater object. 
     
     
       2. The method of  claim 1  further comprising the step of forming a synthetic aperture as the line array of N acoustic sensors moves to get more aperture to increase the measurement accuracy relative to a line array of N acoustic sensors by increasing the measurable difference in the variation in Doppler shifts. 
     
     
       3. The method in  claim 1 , further comprising a method to determine the variation of the Doppler shift due to the motion of the object normal to the line array using the equation 
       
         
           
             
               
                 
                   Δ 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     f 
                     2 
                   
                 
                 - 
                 
                   Δ 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     f 
                     1 
                   
                 
               
               ≅ 
               
                 
                   
                     v 
                     
                       2 
                       ⁢ 
                       c 
                     
                   
                   [ 
                   
                       
                   
                   ⁢ 
                   
                     
                       θ 
                       1 
                       2 
                     
                     - 
                     
                         
                     
                     ⁢ 
                     
                       θ 
                       2 
                       2 
                     
                   
                   ] 
                 
                 . 
               
             
           
         
       
     
     
       4. The method in  claim 3 , further comprising the removal of any frequency shifts due to the motion of the object normal to the line array by fitting the difference in frequency to a line with a least squares fit, thereby more accurately determining the motion of the object parallel to the line array.

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